Gamma radiation field intensity meter

ABSTRACT

A gamma radiation intensity meter measures dose rate of a radiation field. The gamma radiation intensity meter includes a tritium battery emitting beta rays generating a current which is essentially constant. Dose rate is correlated to an amount of movement of an electroscope element charged by the tritium battery. Ionizing radiation decreases the voltage at the element and causes movement. A bleed resistor is coupled between the electroscope support element or electrode and the ionization chamber wall electrode.

This invention was made with Government support under contractDE-AC05-840R21400 and PO 80X-SH104 awarded by the U.S. Department ofEnergy to Martin Marietta Energy Systems, Inc. and the Government hascertain rights in this invention.

This is a division of application Ser. No. 08/044,678 filed Apr. 9,1993, now abandoned.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a gamma radiation field intensitymeter, and more particularly to an electroscope-type dosimeter which issupplied a constant current from an energy source to provide rate ofradiation dose rather than total accumulated dose.

2. Background of the Related Art

Electroscope-type dosimeters have been developed over the years tomeasure the accumulated or total dose of gamma radiation. Specifically,the prior art electroscope-type dosimeter determines the total gammaradiation exposed to it. Typically, the electroscope-type dosimeter,more commonly known as the Lauritsen electroscope, is precharged by aconventional dosimeter charger. The electroscope-type dosimeter includesa quartz fiber and a metal frame used as a charge acceptor, and duringthe charging process a potential is applied between the frame and theexterior of the dosimeter. Electrical charges of the same polarityappear on both the fiber and frame, causing the fiber to be repelledfrom the frame by a distance proportional to the applied voltage. Thechamber walls or exterior of the electroscope-type dosimeter provides anelectrostatic shield for the electroscope-type dosimeter. If theelectroscope-type dosimeter is exposed to additional ionizing gammaradiation, the charge on the quartz fiber decreases and the fiber tendsto return to the discharge position which is closer to the frame. Animage of the fiber in the new position resulting from the additionalgamma radiation is projected onto a reticle scale and viewed through aneyepiece lens of the dosimeter. The scale, typically calibrated inMilliroentgens or Roentgens, indicates total accumulated radiation dose,and may be read by looking through the eyepiece toward a lamp or otherlight source. Thus, the prior art electroscope-type dosimeters have beenunable to measure the radiation dose rate experienced when exposed to anionizing gamma radiation field.

It is, therefore, desirable to reliably measure the radiation dose ratewhich a meter is exposed to in a radiation field to further indicatewhether the ionizing gamma radiation field is dangerous. In addition, itis also desirable that the gamma radiation field intensity meter becompact.

SUMMARY OF THE INVENTION

It is, therefore, an object of the present invention to provide a gammaradiation field intensity meter which is able to measure the dose rateat which the meter is exposed to the ionizing gamma radiation.

It is another object of the present invention to provide a gammaradiation field intensity meter which is compact.

To achieve these and other objects, the gamma radiation intensity meterof the present invention includes a current source generating a currentwhich is essentially constant and a dose rate determining unit whichdetermines the dose rate of the radiation field exposed to the gammaradiation intensity meter. The dose rate determining unit includes anionization chamber having gas, a conductive frame disposed in theionization chamber conducting the current generated by the tritiumbattery and a charge accepting fiber connected to the conductive frame.The gamma radiation intensity meter also includes a resistor, connectedbetween the conductive frame and the ionization chamber wall whichconducts the current forming a potential across the resistor. When thegamma radiation intensity meter is exposed to a radiation field, theradiation field penetrates the gamma radiation intensity meter andionizes the gas in the ionization chamber forming ionized gas, and theionized gas conducts a current proportional to the radiation fieldintensity from the conductive frame to the wall of the ionizationchamber, thereby shunting that amount of current away from the resistor.The reduced current through the resistor proportionally reduces thevoltage on the conductive frame and the fiber and the charge acceptingfiber moves toward the conductive frame to a new position indicating thedose rate.

These, together with other objects and advantages which will besubsequently apparent, reside in the details of construction andoperation as more fully hereinafter described and claimed, withreference being had to the accompanying drawings forming a part hereof,wherein like numerals refer to like parts throughout.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a vertical cross-sectional view of a gamma radiation fieldintensity meter according to a preferred embodiment of the presentinvention;

FIG. 2 is a horizontal cross-sectional view taken along line II--II ofFIG. 1;

FIG. 3 is a wiring schematic diagram of the gamma radiation fieldintensity meter of FIGS. 1 and 2; and

FIG. 4 is a graph showing the relationship between the total current,resistor current, and bleed current.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT

Referring to FIGS. 1 and 2, a radiation field intensity meter 10includes a first electrode 12 made from an electrically conductivematerial, such as a suitable metal. Alternatively, the electrode 12 canbe made of a plastic or other non-conductive material having aconductive coating on the inside thereof.

The electrode 12 is a hollow cylindrical sleeve having opposite axialends 14 and 16. An end plate 15 made of non-conductive material isfixedly disposed in the end 14 and includes a window 15a to permitviewing into the electrode 12. A transparent disk 18 fixedly disposedand hermetically sealed transversely in the electrode 12 at a suitableposition between the opposite ends divides the interior space of theelectrode 12 into an ionization chamber 20 and a battery chamber 22. Thedisk 18 is made of clear plastic, glass or other suitable materials toallow light to pass through the battery chamber 22. A second transparentdisk 24, made of the same type of material as the disk 18, seals thebattery chamber 22, which is evacuated to create a vacuum therein. Also,the transparent material permits light to pass through the batterychamber 22, thus illuminating the interior of the electrode 12.

The disk 18 provides support for a second electrode 26 which is made ofa suitable metallic or otherwise conductive material. The electrode 26has an angled end 26a and supports an electroscope element 28, in theform of a fiber. This arrangement of a fiber and supporting structure or"frame" is standard for a Lauritsen-type electroscope. When theelectrode 26 and element 28 are charged, the position of element 28 withrespect to the end 26a of the electrode 26 varies in accordance with theamount of charge.

The electrode 26 and electroscope element 28 are continuously charged bya fixed, small current from an isotopic battery 30. In the illustratedembodiment, the battery is a beta battery which emits beta radiations(electrons) as a source material decays. A cylindrical support 32,preferably made of conductive metal, is coated with a film 34 of betasource material. For a tritium source, a hydride coating referred to as"tritide" can be used. In other embodiments, the tritium source materialcan be adsorbed into and onto the metal support 32. The tritium sourcebattery illustrated will produce a high open-circuit voltage of, forexample, 18 KV. For still higher voltages, other source materials may beused, such as Ni-63 which produces 63 KV. These sources emit only a lowenergy beta particle and are easily sealed and shielded for completesafety in the present application.

The beta particle emissions are represented by the arrows in FIG. 1, andindicate a current flow to the electrode 12. The current flow is small,such as 2×10⁻¹⁰ amps for about 7 micro-gms of tritium. The currentpasses through a large resistance 36, such as a 10¹² ohm resistor, toproduce an appropriate voltage, such as 200 V (which is the same as theexisting integrated dose dosimeters) for a fully-charged indication onthe electroscope element 28.

When the meter 10 is placed in an ionizing radiation field, a fractionof the battery current linearly proportional to the intensity of theradiation field is shunted through the air-filled ionization chamber 20,and the voltage on the electroscope element 28 is proportionallyreduced. The reduced voltage will cause the element 28 to move towardsthe end 26a of the electrode 26, and this movement can be observed by aperson carrying the meter 10 for an instantaneous indication of the doserate. The movement can be observed and calibrated for dose rate usingconventional observation components found in known portable dosimetersmanufactured by Bendix Corporation and Landsverk Electrometer Companyand sold under the model designations CD V-138, CDE V730, CD V-740 andCD V-742. These components are illustrated in FIG. 1 as an objectivelens 38, an eyepiece lens 40, and a calibrated reticle 42, all of whichare mounted in a barrel 44 which houses all components of the meter 10.The opening 15a makes the electroscope element 28 readable from abovethe disk 14. Moreover, the transparency of both disks 18 and 24 allowslight to pass through the meter 10, thus making the element 28 visiblefor observation.

Referring to FIG. 2, the electrode 26 is connected to the support 32through a spider 46 having four legs. Since the support 32 is hollow, itis preferable to use the spider 46 to interconnect the support 32 to theelectrode 26 so as to allow light to pass therethrough. This enhancesthe readability of the dose rate.

The visual electroscope readout is calibrated in dose-rate and theworker can tell at a glance the degree of danger he is in at the instantof the reading. When in a radiation field, the ionization currentthrough the dosimeter would parallel the resistor 36 and a new, lowerequilibrium voltage would be assumed for each radiation level, thusindicating the strength of the radiation field. If lower electroscopevoltages are desired, smaller sources and lower resistances can be used.

Referring to FIG. 3, the battery 30 produces a current of, for example,2×10⁻¹⁰ amps (I.sub.β) which remains constant. The current through theresistor 36 (I_(R)) with no radiation exposure is the same as the outputcurrent of the battery 30. In the presence of ionizing radiation, acurrent drain is established between the electrode 12 and the electrode26 which causes a drop in the current through the resistor 36 and thus adrop in the potential on the electrode 26 and element 28. This drop is afunction of the amount of ionization, and thus, the element 28 moves inaccordance to the amount of current drained.

The ionization current I.sub.γ thus increases at the expense of resistorcurrent. When the radiation field intensity meter 10 is exposed to gammaradiation, the ionization chamber, which is represented as currentdrain, diverts more of constant current I.sub.β through the ionizationchamber. Accordingly, resistor current I_(R) becomes smaller, andtherefore, less current flows through resistor. Thus, the voltage dropacross resistor decreases, and therefore, the voltage on element 28 inthe ionization chamber is also decreased. As a result of the decrease incharge on the fiber, the fiber moves toward the frame in a new position,thereby indicating radiation dose rate. The volts on the movableelectroscope element or fiber E_(o) =(2×10⁻¹⁰ -V×9.25×10⁻¹⁴ y) 10¹²where V is the ionization chamber volume, y is Roentgens/hr (R/hr).

Referring to FIG. 4, the current flowing from the current source, i.e.the beta battery, remains constant at, for example, 2×10⁻¹⁰ ampsthroughout a range of radiation exposure. The resistance of the resistoris fixed at, for example, 10¹² ohms. The current through the ionizationchamber increases substantially linearly as the gamma radiation exposureincreases. Given the above, one can easily calibrate a reticle tocorrelate voltage and thus fiber position to dose rate in R per hour, asshown on the horizontal axis of FIG. 4.

While the present invention is particularly well suited for detectinggamma radiation, it can be used to detect other electromagneticionization radiations, such as X-rays. Moreover, while the describedembodiments focus on beta radiation batteries, alpha battaries can alsobe employed. In any event, the isotopic source material can be placed onthe carrier in any convenient manner, such as a coating or having thesource material adsorbed on the surface.

The many features and advantages of the invention are apparent from thedetailed specification, and thus, it is intended by the appended claimsto cover all such features and advantages of the invention which fallwithin the true spirit and scope of the invention. For example, thepresent invention is not limited to the tritium battery, but can be usedwith any constant current source such as a Ni-63 battery or anelectronic current source. Further, since numerous modifications andvariations will readily occur to those skilled in the art, it is notdesired to limit the invention to the exact construction and operationillustrated and described, and accordingly, all suitable modificationsand equivalents may be resorted to, falling within the scope of thepresent invention.

What is claimed is:
 1. A battery for an electroscope comprising:anevacuated battery chamber having a support disposed therein and beinglight transmissive therethrough; a substantially open-ended hollowmember connected to the support and being light transmissivetherethrough; and an isotopic source material carried by the hollowmember and emitting charged particles across an annular evacuated gaponto the wall of the evacuated battery chamber.
 2. A battery accordingto claim 1, wherein the source material is tritium coated on a surfaceof the hollow member.
 3. A battery according to claim 1, wherein thehollow member is cylindrical and substantially coaxial with theevacuated battery chamber.
 4. A battery for an electroscope comprising:afirst electrode having a hollow, substantially cylindrical form; asecond electrode having a hollow, substantially cylindrical form andbeing arranged coaxially with respect to the first electrode; anisotopic source material carried by one of the first and secondelectrodes; and a chamber containing the one electrode carrying theisotopic source material, and being formed at least partially by firstand second substantially, spaced apart light transmissive membersdisposed at opposite axial ends of the chamber.
 5. A battery accordingto claim 4, wherein the first electrode is supported in electricalisolation from the second electrode by one of the first and secondtransparent members.
 6. battery according to claim 4, wherein the sourcematerial is tritium coated on an outer surface of an inner one of thefirst and second electrodes.
 7. A battery according to claim 4, whereinthe chamber is evacuated.